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If a reaction follows the Arrhenius equa...

If a reaction follows the Arrhenius equation, the plot lnk vs 1/RT gives a straight-line having intercept 'In a' unit on positive y-axis. The maximum value of rate constant k is :

A

`-a` unit

B

a R unit

C

a unit

D

a/R unit

Text Solution

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The correct Answer is:
To solve the problem, we will use the Arrhenius equation and analyze the relationship between the rate constant \( k \) and temperature \( T \). ### Step-by-Step Solution: 1. **Understand the Arrhenius Equation**: The Arrhenius equation is given by: \[ k = A e^{-\frac{E_a}{RT}} \] where: - \( k \) = rate constant - \( A \) = pre-exponential factor (frequency factor) - \( E_a \) = activation energy - \( R \) = universal gas constant - \( T \) = temperature in Kelvin 2. **Take the Natural Logarithm**: Taking the natural logarithm of both sides gives: \[ \ln k = \ln A - \frac{E_a}{RT} \] 3. **Rearranging the Equation**: We can rearrange this equation to match the form of a straight line \( y = mx + c \): \[ \ln k = -\frac{E_a}{R} \cdot \frac{1}{T} + \ln A \] Here, we can identify: - \( y = \ln k \) - \( x = \frac{1}{T} \) - \( m = -\frac{E_a}{R} \) (slope) - \( c = \ln A \) (y-intercept) 4. **Identify the Maximum Value of \( k \)**: The maximum value of \( k \) occurs when the term \( -\frac{E_a}{RT} \) is minimized. This happens when \( T \) approaches infinity (as \( R \) is constant). 5. **Limit as \( T \to \infty \)**: As \( T \) approaches infinity: \[ \frac{1}{T} \to 0 \] Therefore, the equation simplifies to: \[ \ln k = \ln A \] This implies: \[ k = A \] 6. **Conclusion**: The maximum value of the rate constant \( k \) is: \[ k_{\text{max}} = A \] ### Final Answer: The maximum value of the rate constant \( k \) is \( A \).

To solve the problem, we will use the Arrhenius equation and analyze the relationship between the rate constant \( k \) and temperature \( T \). ### Step-by-Step Solution: 1. **Understand the Arrhenius Equation**: The Arrhenius equation is given by: \[ k = A e^{-\frac{E_a}{RT}} ...
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